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Slide 1 Problem of Coleman-Mazur on p-adic families of L-functions
Problem of Coleman-Mazur on p-adic families
of L-functions
A. A. Panchishkin?
Institut Fourier, B.P.74, 38402 St.–Martin d’Hères, FRANCE
e-mail : panchish@mozart.ujf-grenoble.fr, FAX: 33 (0) 4 76 51 44 78
Slide 1
Abstract
For a prime number p ≥ 5, consider a primitive cusp
eigenform f = fk of weight k ≥ 2, f =
P∞
n=1 anq
n, and consider
a family of cusp eigenforms fk′ of weight k′ ≥ 2,
k′ 7→ fk′ =
P∞
n=1 an(k
′)qn, containing f for k′ = k, such that
the Fourier coefficients an(k′) are given by certain p-adic
analytic functions k′ 7→ an(k′) for (n, p) = 1, and let αp(k′) be a
Satake p-parameter of fk′ .
In The Eigencurve (1998), R.Coleman and B.Mazur stated
the following problem:
Given a prime p and a family {fk′} of cusp eigenforms of a
fixed positive slope σ = ordp(αp(k′)) 0, to construct a two
variable p-adic L-function interpolating on all k′ the Amice-Vélu
p-adic L-functions Lp(fk′) studied in [Am-Ve] , [Vi76] and in
[MTT].
A solution (2003, see [PaTV]) is described using the
Rankin-Selberg method and the theory of p-adic integration with
values in a p-adic Banach algebra A.
?A talk held in Kyoto on September 22, 2005, 10:30–12:00.
Slide 2
Our p-adic L-functions are Mellin transforms of certain
measures with values in A. We construct such measures from
products of classical Eisenstein series, which produce
distributions with values in certain Banach A-modules
M = M(N ; A) of modular forms with coefficients in the algebra
A.
Another approach, based on modular symbols, was
developed by Glenn Stevens. Applications of these results to the
p-adic Birch and Swinnerton-Dyer conjecture were discussed by
P.Colmez (Bourbaki talk, June 2003, [Colm03]).
Contents
0 Statement of the problem of Coleman-Mazur 4
Slide 3
1 p-adic integration and the p-adic weight space 18
2 Coleman’s families 26
3 Main results 31
4 Construction of the admissible measure μ? 36
5 Criterion of admissibility 40
6 Modular Eisenstein distributions Φj 43
7 Algebraic A-linear form `α : MN (ψ;A)α → A 48
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